In: Physics
use the thin lens equation to explain why for a given screen-object distance there are two positions where the image is in focus
The the light rays follow the same path through a lens whether coming from the left or right - it is called the principle of reversibility. The lens can be turned around and would still work just the same. If the object is x cm from one side of the Lens and y cm from the other side, turning the lens around will simply reverse x and y values. The object-screen distance (x+y) is unchanged. So for a given object-screen distance, there are two positions where the image is in focus
Using several different measured object lengths and their
corresponding image lengths, we will find the focal length of a
lens, as well as verify the characteristics of the image (location,
height, virtual or real, inverted or right-side up) for each object
distance. This data will be used to prove that the thin lens
equation is true.
Hypothesis and Rationale: By plotting the inverse of the object
distances and the inverse of the corresponding image distances on a
graph, the inverse of the x-intercept and the slope of the
resulting graph will be equal to the focal length of our lens. We
know this based on the equation 1/f=1/di + 1/do.
Methods and Materials: To do this experiment, we began with an
optical bench which we placed on a flat surface (our desk). Then,
we attached our object (the light source) to the optical bench
where distance=0cm. It is important that we aimed the light source
so that the image (ours was two parallel arrows) down the optical
bench. This allows us to measure the object distance with ease.
Then we placed a blank white screen on the opposite end of the
optical bench from the light source where the image was facing.
Finally, we placed a thin lens holder in the middle, and turned on
the light source by plugging it into a power outlet. In order to
get the data necessary, we placed the lens holder in a position
that is between the light source and the screen, and moved the
screen to a position where there was a clear image that is similar
to the object on the light source (the image should be VERY CLEAR).
We measured and recorded the distance of the lens holder from the
light source(Do)
as well as the lens holder from the screen(Di).
Then we moved the lens holder to an other position between the
light source and screen, found where the new image appeared with
the screen and recorded the same measurements. We repeated this
process for 10 specific and different locations of the lens holder,
using these points to generate our graph.